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Damage formation and annealing studies of low energy ion implants ...

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4.5 Sample product<strong>ion</strong><br />

Samples have been implanted using an Applied Materials Quantum LEAP<br />

implanter (12) at AMD Dresden <strong>and</strong> Applied Materials (UK). Some samples <strong>and</strong> have<br />

also been implanted at Salford University using the ultra <strong>low</strong> <strong>energy</strong> (ULE) implanter<br />

(11). The principle behind the two implanters is the same <strong>and</strong> the Salford implanter is<br />

described here in sect<strong>ion</strong> 4.5.1. Major differences between them are the size <strong>of</strong> sample<br />

that can be implanted <strong>and</strong> sample throughput. The implanter at Salford is a research tool<br />

<strong>and</strong> can only implant small samples <strong>of</strong> approximately 12 × 12 mm. The Applied<br />

implanter is a manufacturing tool <strong>and</strong> hence wafers <strong>of</strong> 200mm or 300mm diameter were<br />

implanted. Unless otherwise stated, the <strong>implants</strong> used in this thesis were implanted at<br />

AMD. Annealing was carried out at Salford University using an Steag AST 10 RTP<br />

system, <strong>and</strong> at AMD using an Applied Materials RTP Radiance system. These are both<br />

lamp based tools.<br />

4.5.1 Salford Ultra Low Energy Implanter Laboratory<br />

A schematic <strong>of</strong> the ULE implanter (11) is shown in Figure 4.23. The beamline<br />

consists <strong>of</strong> three electrically isolated sect<strong>ion</strong>s; the <strong>ion</strong> source, beam transport, <strong>and</strong> target<br />

chamber. Two Applied Materials <strong>ion</strong> source assemblies are located symmetrically about<br />

a mass analysing magnet. The <strong>ion</strong> sources used are the Bernas type, fitted with ovens<br />

for solid source materials <strong>and</strong> also several gas inputs. The sources have a triode<br />

extract<strong>ion</strong> system, with adjustable gap <strong>and</strong> lateral alignment, which can adjust the<br />

pr<strong>of</strong>ile <strong>of</strong> the beam.<br />

Beams are selected by focusing them through an adjustable mass resolving slit<br />

located beyond the mass analysing magnet. Any neutrals present in the beam are<br />

removed in a second magnet used to bend the beam through 5 º or 90 º into one <strong>of</strong> two<br />

target chambers. For implantat<strong>ion</strong> the target chamber is used. The system comprises <strong>of</strong><br />

five stages <strong>of</strong> differential pumping so that pressures <strong>of</strong> ~ 10 -8 mbar are maintained in the<br />

target chambers while the sources operate at ~ 10 -4 mbar. In the target chamber used for<br />

the <strong>implants</strong> is a target mount attached to a precis<strong>ion</strong> goniometer with one rotat<strong>ion</strong>al <strong>and</strong><br />

three direct<strong>ion</strong>al degrees <strong>of</strong> freedom. At the final stage a <strong>low</strong> fill factor decelerat<strong>ion</strong> lens<br />

is located directly in front <strong>of</strong> the target. The lens al<strong>low</strong>s beams to be transported at<br />

higher energies (5 – 15 keV) before being decelerated at the target to energies as <strong>low</strong> as<br />

20 eV. This set up is called accel – decel mode, also referred to as retard mode.<br />

Alternatively the transport <strong>and</strong> target sect<strong>ion</strong>s may be electrically coupled so that <strong>ion</strong>s<br />

100

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